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Shallow Characters and Supercuspidal Representations

Stella Sue Gastineau
[email protected]
Abstract

In 2014, Reeder and Yu constructed epipelagic representations of a reductive pp-adic group GG from stable functions on shallowest Moy-Prasad quotients. In this paper, we extend these methods when GG is split. In particular, we classify all complex-valued characters vanshing on a slightly deeper Moy-Prasad subgroup and show that, while sufficient, a naive extension of Reeder-Yu’s stability condition is not necessary for constructing supercuspidal representations.

1 Introduction

1.1 Notation

Let kk be a non-archimedean local field with value group \mathbb{Z} and ring of integers 𝔬\mathfrak{o} with prime ideal 𝔭\mathfrak{p} and residue field 𝔣:=𝔬/𝔭\mathfrak{f}:=\mathfrak{o}/\mathfrak{p} of finite cardinality qq and characteristic pp. Let KK be a maximal unramified extension of kk, with algebraically closed residue field 𝔉\mathfrak{F}. Let 𝐆\mathbf{G} be an absolutely simple, simply connected algebraic group defined and splitting over kk. We fix the following subgroups of 𝐆\mathbf{G} for consideration:

  • 𝐓\mathbf{T} a maximal torus, defined and splitting over kk.

  • 𝐁\mathbf{B} a Borel subgroup of 𝐆\mathbf{G}, containing 𝐓\mathbf{T} and defined over kk.

  • 𝐔\mathbf{U} the unipotent radical of 𝐁\mathbf{B}, defined over kk.

We will also use unbolded letters G,B,T,UG,B,T,U to denote the kk-rational points of 𝐆,𝐁,𝐓,𝐔\mathbf{G},\mathbf{B},\mathbf{T},\mathbf{U} respectively. We will be assuming the basic structure of such groups, which can be found in [3, 5].

1.2 Motivation

The group GG acts on its Bruhat-Tits building =(𝐆,k)\mathcal{B}=\mathcal{B}(\mathbf{G},k) and for each point λ\lambda\in\mathcal{B}, the stabilizer P:=GλP:=G_{\lambda} has a filtration by open Moy-Prasad subgroups:

P>Pr1>Pr2>P>P_{r_{1}}>P_{r_{2}}>\cdots

indexed by an increasing, discrete sequece 𝐫(λ)=(r1,r2,)\mathbf{r}(\lambda)=(r_{1},r_{2},\dots) of positive real numbers. The first Moy-Prasad subgroup Pr1P_{r_{1}} is called the pro-unipotent radical of PP, and will be denoted by P+P_{+}. In their papers, Gross-Reeder [2] and Reeder-Yu [4] study complex characters of

χ:P+×\chi:P_{+}\to\mathbb{C}^{\times}

that are trivial on the Moy-Prasad subgroup Pr2P_{r_{2}}. In this paper we will go a little bit deeper down the Moy-Prasad filtration and classify all shallow characters, those being characters that are trivial on Moy-Prasad subgroup P1Pr2P_{1}\subseteq P_{r_{2}}.

In §2.2, we show that a shallow character on P+P_{+} can be recovered from its restrictions to its affine root subgroups and extended to a group homomorphism. In particular, in Theorem 4 we show that in order to to define a shallow character, it is both necessary and sufficient that the extension be trivial on commutators

[Uβ,Uα]i,j>0Uiα+jβ[U_{\beta},U_{\alpha}]\subseteq\prod_{i,j>0}U_{i\alpha+j\beta}

where α\alpha and β\beta are affine roots whose gradients are not linearly dependant.

Following a classification of shallow characters, we ask for which shallow characters χ:P+×\chi:P_{+}\to\mathbb{C}^{\times} is the compactly-induced representation

indP+G(χ)={ϕ:G|ϕ(hx)=χ(h)ϕ(x)ϕ compactly supported}\operatorname{ind}_{P_{+}}^{G}(\chi)={\small\left\{\phi:G\to\mathbb{C}~{}\left|~{}\begin{gathered}\text{$\phi(hx)=\chi(h)\cdot\phi(x)$}\\ \text{$\phi$ compactly supported}\end{gathered}\right\}\right.}

a supercuspidal representation of GG. In their papers, Gross-Reeder and Reeder-Yu give a classification of supercuspidal representations of GG via stable orbits in a related graded Lie algebra. In Proposition 8 of §3.2, we look at a naive generalization of [4, Propositio 2.4] and show that it is sufficient but not necessary for determining which shallow characters induce up to supercuspidal representations of GG.

2 Shallow Characters

Throughout this paper we will fix an alcove of the apartment 𝒜\mathcal{A}\subseteq\mathcal{B} corresponding to TT, and we will let

Δ={α0,α1,,α}\Delta=\{\alpha_{0},\alpha_{1},\dots,\alpha_{\ell}\}

denote the corresponding set of simple affine roots. We will also fix a point λ\lambda contained in the closure of this alcove. We will denote by J𝒜\mathcal{F}_{J}\subseteq\mathcal{A} the facet containing λ\lambda given by the non-vanishing of the simple affine roots ΔJΔ\Delta_{J}\subseteq\Delta, where

J{0,1,,,}.J\subsetneq\{0,1,,\dots,\ell\}.

We will also let P=GλP=G_{\lambda} denote the stabilizer of λ\lambda in GG.

2.1 Shallow affine roots

Given an affine root α:𝒜\alpha:\mathcal{A}\to\mathbb{R}, we say that its depth (at λ\lambda) is the real number α(λ)\alpha(\lambda). Then we say that α\alpha is shallow (at λ)\lambda) if its depth is strictly between 0 and 11. We also say that α\alpha is decomposable (as a shallow affine root) if there exists another shallow affine root β\beta such that αβ\alpha-\beta is a shallow affine root. Otherwise, we say that α\alpha is indecomposable (as a shallow affine root).

Note that the depth of a shallow affine root precisely depends on λ\lambda; whereas, the set of decomposable and indecomposable shallow affine roots depend only on the the facet J\mathcal{F}_{J} and not on the point λ\lambda itself. In fact, setting

nJ(n0α0+n1α1++nα):=jJnjn_{J}(n_{0}\alpha_{0}+n_{1}\alpha_{1}+\cdots+n_{\ell}\alpha_{\ell}):=\sum_{j\in J}n_{j}

for njn_{j}\in\mathbb{Z}, we can characterize the indecomposable shallow affine roots as follows:

Lemma 1.

A shallow affine root α\alpha is indecomposable if and only if nJ(α)=1n_{J}(\alpha)=1.

Proof.

Let α\alpha be a shallow root. First note that if nJ(α)=1n_{J}(\alpha)=1, then α\alpha must be indecomposable as a shallow affine root: Indeed, if β,αβ\beta,\alpha-\beta is an affine root, then exactly one of αβ\alpha-\beta and β\beta is shallow since

nJ(αβ)=nJ(α)nJ(β).n_{J}(\alpha-\beta)=n_{J}(\alpha)-n_{J}(\beta).

Therefore, for the remainder of the proof we suppose that nJ(α)2n_{J}(\alpha)\geq 2.

First write

α=αi1+αi2++αim,\alpha=\alpha_{i_{1}}+\alpha_{i_{2}}+\cdots+\alpha_{i_{m}},

so that

βj\displaystyle\beta_{j} =αi1++αij\displaystyle=\alpha_{i_{1}}+\cdots+\alpha_{i_{j}}
αβj\displaystyle\alpha-\beta_{j} =αij+1++αim\displaystyle=\alpha_{i_{j+1}}+\cdots+\alpha_{i_{m}}

are an affine roots for all j=1,2,,mj=1,2,\dots,m. Such a decomposition is possible, for example, by Lemma 3.6.2 in [1]. Since nJ(α)2n_{J}(\alpha)\geq 2, we know that there exists a j=1,2,,mj=1,2,\dots,m such that both βj\beta_{j} and αβj\alpha-\beta_{j} are shallow. For instance, we can choose jj to be minimal such that αij\alpha_{i_{j}} is a shallow affine root in ΔJ\Delta_{J}. Thus, by setting β=βj\beta=\beta_{j}, we have given a decomposition

α=β+(αβ)\alpha=\beta+(\alpha-\beta)

as shallow affine root whenever nJ(α)2n_{J}(\alpha)\geq 2. ∎

Lemma 2.

Suppose that α,β\alpha,\beta are shallow affine roots such that there are positive integers i,j>0i,j>0 such that iα+jβi\alpha+j\beta are shallow affine roots. Then α+β\alpha+\beta is a shallow affine root.

Proof.

Suppose that iα+jβi\alpha+j\beta is a shallow affine root for positive integers i,j>0i,j>0. If both i,j=1i,j=1, then α+β\alpha+\beta is a shallow affine root and we are done. Therefore, without loss of generality, we will assume that i>0i>0. Note that in this case, we then have the following chain of inequalities:

0<α(λ)<α(λ)+β(λ)<iα(λ)+jβ(λ)<1.0<\alpha(\lambda)<\alpha(\lambda)+\beta(\lambda)<i\alpha(\lambda)+j\beta(\lambda)<1. (2.1)

Thus, if we can show that α+β\alpha+\beta is an affine root, then it must be shallow.

First, we note that α+β\alpha+\beta cannot be a constant function. Since GG is split, the minimal relation of the affine root group is of the form

1=m0α0+m1α1++mα.1=m_{0}\alpha_{0}+m_{1}\alpha_{1}+\cdots+m_{\ell}\alpha_{\ell}.

In particular, if α+β\alpha+\beta was a positive constant function, then it must take value at least 11. But this contradicts the inequalities in (2.1).

Let a,ba,b be the respective gradients of α,β\alpha,\beta. The subroot system of RR generated by aa and bb must have rank at most 22. In fact, its rank must be exactly 22, since α+β\alpha+\beta is not a constant function. We know that this rank 2 subsystem is not of type 𝐀2\mathbf{A}_{2}, since we are assuming that ia+jbia+jb is a root for i>1i>1. Therefore, we only need to consider the case where aa and bb generate a root system of type 𝐂2\mathbf{C}_{2} or 𝐆2\mathbf{G}_{2}. In both cases, one can check directly that if ia+jbia+jb is a root for positive integers i,ji,j then a+ba+b is a root as well. ∎

2.2 Shallow characters

A shallow character of the pro-unipotent radical P+PP_{+}\subseteq P is any group homomorphism

χ:P+×\chi:P_{+}\to\mathbb{C}^{\times}

that is trivial on the the Moy-Prasad subgroup

P1=T0,Uαα(λ)1,P_{1}=\left\langle T_{0},U_{\alpha}\mid\alpha(\lambda)\geq 1\right\rangle,

where T0=𝐓(1+𝔭)T_{0}=\mathbf{T}(1+\mathfrak{p}) is the maximal compact subgroup of TT and UαU_{\alpha} is the affine root subgroup of GG corresponding to the affine root α\alpha. Since P1P_{1} is a normal subgroup of P+P_{+}, any shallow character of P+P_{+} must factor through the quotient P+/P1P_{+}/P_{1}, a finite group generated by subgroups

UαP1/P1Uα/Uα+1𝔣U_{\alpha}P_{1}/P_{1}\cong U_{\alpha}/U_{\alpha+1}\cong\mathfrak{f}

with α\alpha being shallow affine roots. Indeed, given any coset gP1gP_{1} in P+/P1P_{+}/P_{1}, there is a unique decomposition

gP1=(αuα(xα)P1),gP_{1}=\left(\prod_{\alpha}u_{\alpha}(x_{\alpha})P_{1}\right), (2.2)

where the product is relative to some fixed order over all shallow affine roots α\alpha [5, §3.1.1]. Therefore, any shallow character χ\chi can be recovered from its restriction to the shallow affine root groups via the formula:

χ(gP1):=αχα(x¯α),\chi(gP_{1}):=\prod_{\alpha}\chi_{\alpha}(\bar{x}_{\alpha}),

where χα:𝔣×\chi_{\alpha}:\mathfrak{f}\to\mathbb{C}^{\times} is the additive character defined by setting

χα(x¯):=χ(uα(x)P1)\chi_{\alpha}(\bar{x}):=\chi(u_{\alpha}(x)P_{1})

for any lift x𝔬x\in\mathfrak{o} of x¯𝔣\bar{x}\in\mathfrak{f}.

Lemma 3.

Let χ:P+/P1×\chi:P_{+}/P_{1}\to\mathbb{C}^{\times} be a shallow character of P+P_{+} given by additive characters as above. Then for any shallow affine roots α,β\alpha,\beta we have the following identities:

1=i,jχiα+jβ(Cαβijx¯iy¯j),1=\prod_{i,j}\chi_{i\alpha+j\beta}(C_{\alpha\beta ij}\bar{x}^{i}\bar{y}^{j}),

where the product is over all i,j>0i,j>0 such that iα+jβi\alpha+j\beta is a shallow affine root and the constants CαβijC_{\alpha\beta ij} are given as in the Chevalley Commutator Formula [1, Theorem 5.2.2].

Proof.

Let α,β\alpha,\beta be two shallow affine roots such that iα+jβi\alpha+j\beta is a shallow affine root for some positive integers i,j>0i,j>0. Then by Lemma 2, we know that α+β\alpha+\beta is a shallow affine root. Therefore, we can apply the Chevalley commutator formula [1, Theorem 5.2.2], which says that

[uβ(y),uα(x)]P1=i,juiα+jβ(Cαβijxiyj)P1[u_{\beta}(y),u_{\alpha}(x)]P_{1}=\prod_{i,j}u_{i\alpha+j\beta}(C_{\alpha\beta ij}x^{i}y^{j})P_{1}

for all x,y𝔬x,y\in\mathfrak{o}. Here the product is in increasing order over all i,j>0i,j>0 such that iα+jβi\alpha+j\beta is an affine root. But if any iα+jβi\alpha+j\beta is not shallow, then Uiα+jβP1U_{i\alpha+j\beta}\subseteq P_{1}. Therefore, we can assume that the product is only over i,j>0i,j>0 such that iα+jβi\alpha+j\beta is a shallow affine root.

Now let χ:P+/P1×\chi:P_{+}/P_{1}\to\mathbb{C}^{\times} be any shallow character of P+P_{+}. Since χ\chi is a group homomorphism, we know that

χ([uβ(y),uα(x)]P1)\displaystyle\chi([u_{\beta}(y),u_{\alpha}(x)]P_{1}) =i,jχ(uiα+jβ(Cαβijxiyj)P1)\displaystyle=\prod_{i,j}\chi(u_{i\alpha+j\beta}(C_{\alpha\beta ij}x^{i}y^{j})P_{1})
=i,jχiα+β(Cαβijx¯iy¯j)\displaystyle=\prod_{i,j}\chi_{i\alpha+\beta}(C_{\alpha\beta ij}\bar{x}^{i}\bar{y}^{j})

where the product is over all i,j>0i,j>0 such that iα+jβi\alpha+j\beta is a shallow affine root. Finally, since χ\chi maps into an abelian group ×\mathbb{C}^{\times}, we know that

χ([uβ(y),uα(x)]P1)=1,\chi([u_{\beta}(y),u_{\alpha}(x)]P_{1})=1,

finishing our proof. ∎

Theorem 4.

Suppose that for each shallow affine root α\alpha, we are given an additive character χα:𝔣×\chi_{\alpha}:\mathfrak{f}\to\mathbb{C}^{\times}. Suppose further that for each pair of shallow affine roots α,β\alpha,\beta we have the following relation:

1=i,jχiα+jβ(Cαβijx¯iy¯j),1=\prod_{i,j}\chi_{i\alpha+j\beta}(C_{\alpha\beta ij}\bar{x}^{i}\bar{y}^{j}), (2.3)

where the product is over all i,j>0i,j>0 such that iα+jβi\alpha+j\beta is a shallow affine root. Then there exists a unique shallow character χ:P+/P1×\chi:P_{+}/P_{1}\to\mathbb{C}^{\times} such that

χ(uα(x)P1)=χα(x¯)\chi(u_{\alpha}(x)P_{1})=\chi_{\alpha}(\bar{x}) (2.4)

for all x𝔬x\in\mathfrak{o} and shallow affine root α\alpha. Moreover, any shallow affine root is of this form.

Proof.

For the proof of this theorem, we will fix an enumeration of the shallow affine roots α1,,αn\alpha_{1},\dots,\alpha_{n} so that i<ji<j whenever αi(λ)<αj(λ)\alpha_{i}(\lambda)<\alpha_{j}(\lambda). Then we construct the well-defined function χ:P+/P1×\chi:P_{+}/P_{1}\to\mathbb{C}^{\times} by setting

χ(i=1nuαi(xi)P1):=i=1nχαi(x¯i)\chi\left(\prod_{i=1}^{n}u_{\alpha_{i}}(x_{i})P_{1}\right):=\prod_{i=1}^{n}\chi_{\alpha_{i}}(\bar{x}_{i}) (2.5)

for all x1,,xn𝔬x_{1},\dots,x_{n}\in\mathfrak{o}. Indeed, this function is well-defined since each coset in P+/P1P_{+}/P_{1} has a unique decomposition of the form (2.2) with respect to this shallow affine root ordering. What follows is a proof that χ\chi defines a group homomorphism, and thus, is the unique shallow character satisfying (2.4). Since P+/P1P_{+}/P_{1} is generated by the subgroups UαP1/P1U_{\alpha}P_{1}/P_{1} for shallow affine roots, it will be sufficient to show that

χ(guα(x)P1)=χ(gP1)χα(x¯)\chi(gu_{\alpha}(x)P_{1})=\chi(gP_{1})\cdot\chi_{\alpha}(\bar{x}) (2.6)

for all cosets gP1gP_{1} in P+/P1P_{+}/P_{1} and all shallow affine roots α\alpha.

Let α=αj\alpha=\alpha_{j} be a shallow affine root. We now show that (2.6) holds via descending induction on jj. For the base case, we let j=nj=n so that

χ([i=1nuαi(xi)P1]uαn(x)P1)\displaystyle\chi\left(\left[\prod_{i=1}^{n}u_{\alpha_{i}}(x_{i})P_{1}\right]u_{\alpha_{n}}(x)P_{1}\right) =χ([i=1n1uαi(xi)P1]uαn(xn+x)P1)\displaystyle=\chi\left(\left[\prod_{i=1}^{n-1}u_{\alpha_{i}}(x_{i})P_{1}\right]u_{\alpha_{n}}(x_{n}+x)P_{1}\right)
=[i=1n1χαi(x¯i)]χαn(x¯n+x¯)\displaystyle=\left[\prod_{i=1}^{n-1}\chi_{\alpha_{i}}(\bar{x}_{i})\right]\cdot\chi_{\alpha_{n}}(\bar{x}_{n}+\bar{x})
=[i=1nχαi(x¯i)]χαn(x¯)\displaystyle=\left[\prod_{i=1}^{n}\chi_{\alpha_{i}}(\bar{x}_{i})\right]\cdot\chi_{\alpha_{n}}(\bar{x})

for all x1,,xn,x𝔬x_{1},\dots,x_{n},x\in\mathfrak{o}. For the induction step, assume that

χ(guαi(x)P1)=χ(gP1)χαi(x¯)\chi(gu_{\alpha_{i}}(x)P_{1})=\chi(gP_{1})\cdot\chi_{\alpha_{i}}(\bar{x})

for all cosets gP1gP_{1} in P+/P1P_{+}/P_{1} and every shallow affine root αi\alpha_{i} with i>ji>j. In this case, we look at products of the form

[i=1nuαi(xi)P1]uαj(x)P1=[i=1j1uαi(xi)P1]uαj(xj+x)P1[i=j+1nuαi(xi)[uαj(x),uαi(xi)]P1]\left[\prod_{i=1}^{n}u_{\alpha_{i}}(x_{i})P_{1}\right]u_{\alpha_{j}}(x)P_{1}=\left[\prod_{i=1}^{j-1}u_{\alpha_{i}}(x_{i})P_{1}\right]u_{\alpha_{j}}(x_{j}+x)P_{1}\left[\prod_{i=j+1}^{n}u_{\alpha_{i}}(x_{i})[u_{\alpha_{j}}(x),u_{\alpha_{i}}(x_{i})]P_{1}\right]

If αi+αj\alpha_{i}+\alpha_{j} is a constant, then

[uαj(x),uαi(xi)]P1=P1.[u_{\alpha_{j}}(x),u_{\alpha_{i}}(x_{i})]P_{1}=P_{1}.

Otherwise, we can use the Chevalley commutator formula to say that

[uαj(x),uαi(xi)]P1=k,lukαj+lαi(Cαjαiklxkxil)P1[u_{\alpha_{j}}(x),u_{\alpha_{i}}(x_{i})]P_{1}=\prod_{k,l}u_{k\alpha_{j}+l\alpha_{i}}(C_{\alpha_{j}\alpha_{i}kl}x^{k}x_{i}^{l})P_{1}

where the product is in increasing order over over all k,l>0k,l>0 such that kαj+lαik\alpha_{j}+l\alpha_{i} is a shallow affine root. Note that each such kαj+lαik\alpha_{j}+l\alpha_{i} must occur later than αi\alpha_{i} in the enumeration of shallow affine roots since kαj(λ)+lαi(λ)>αj(λ)k\alpha_{j}(\lambda)+l\alpha_{i}(\lambda)>\alpha_{j}(\lambda). By repeadily applying the induction hypothesis and using relation (2.3), we have that

χ(g[uαj(x),uαi(xi)]P1)=χ(gP1)(k,lχkαj+lαi(Cαjαiklx¯kx¯il))=χ(gP1)\chi(g[u_{\alpha_{j}}(x),u_{\alpha_{i}}(x_{i})]P_{1})=\chi(gP_{1})\left(\prod_{k,l}\chi_{k\alpha_{j}+l\alpha_{i}}(C_{\alpha_{j}\alpha_{i}kl}\bar{x}^{k}\bar{x}_{i}^{l})\right)=\chi(gP_{1}) (2.7)

for all cosets gP1gP_{1} in P+/P1P_{+}/P_{1}. Thus, repeatedly applying the induction hypothesis and (2.7), we have

χ([i=1nuαi(xi)P1]uαj(x)P1)=χ([i=1j1uαi(xi)P1]uαj(xj+x)P1[i=j+1nuαi(xi)[uαj(x),uαi(xi)]P1])=χ([i=1j1uαi(xi)P1]uαj(xj+x)P1[i=j+1n1uαi(xi)[uαj(x),uαi(xi)]P1]uαn(xn)P1)=χ([i=1j1uαi(xi)P1]uαj(xj+x)P1[i=j+1n1uαi(xi)[uαj(x),uαi(xi)]P1])χαn(x¯n)=χ([i=1j1uαi(xi)P1]uαj(xj+x)P1)[i=j+1n1χαi(x¯i)].\chi\left(\left[\prod_{i=1}^{n}u_{\alpha_{i}}(x_{i})P_{1}\right]u_{\alpha_{j}}(x)P_{1}\right)\\ \begin{aligned} &=\chi\left(\left[\prod_{i=1}^{j-1}u_{\alpha_{i}}(x_{i})P_{1}\right]u_{\alpha_{j}}(x_{j}+x)P_{1}\left[\prod_{i=j+1}^{n}u_{\alpha_{i}}(x_{i})[u_{\alpha_{j}}(x),u_{\alpha_{i}}(x_{i})]P_{1}\right]\right)\\ &=\chi\left(\left[\prod_{i=1}^{j-1}u_{\alpha_{i}}(x_{i})P_{1}\right]u_{\alpha_{j}}(x_{j}+x)P_{1}\left[\prod_{i=j+1}^{n-1}u_{\alpha_{i}}(x_{i})[u_{\alpha_{j}}(x),u_{\alpha_{i}}(x_{i})]P_{1}\right]u_{\alpha_{n}}(x_{n})P_{1}\right)\\ &=\chi\left(\left[\prod_{i=1}^{j-1}u_{\alpha_{i}}(x_{i})P_{1}\right]u_{\alpha_{j}}(x_{j}+x)P_{1}\left[\prod_{i=j+1}^{n-1}u_{\alpha_{i}}(x_{i})[u_{\alpha_{j}}(x),u_{\alpha_{i}}(x_{i})]P_{1}\right]\right)\cdot\chi_{\alpha_{n}}(\bar{x}_{n})\\ &\mathmakebox[width("{}={}")][c]{\vdots}\\ &=\chi\left(\left[\prod_{i=1}^{j-1}u_{\alpha_{i}}(x_{i})P_{1}\right]u_{\alpha_{j}}(x_{j}+x)P_{1}\right)\left[\prod_{i=j+1}^{n-1}\chi_{\alpha_{i}}(\bar{x}_{i})\right].\\ \end{aligned}

Finally, using the definition of χ\chi given in (2.5), we arrive at

χ([i=1nuαi(xi)P1]uαj(x)P1)\displaystyle\chi\left(\left[\prod_{i=1}^{n}u_{\alpha_{i}}(x_{i})P_{1}\right]u_{\alpha_{j}}(x)P_{1}\right) =χ([i=1j1uαi(xi)P1]uαj(xj+x)P1)[i=j+1n1χαi(x¯i)]\displaystyle=\chi\left(\left[\prod_{i=1}^{j-1}u_{\alpha_{i}}(x_{i})P_{1}\right]u_{\alpha_{j}}(x_{j}+x)P_{1}\right)\left[\prod_{i=j+1}^{n-1}\chi_{\alpha_{i}}(\bar{x}_{i})\right]
=[i=1j1χαi(x¯i)]χαj(x¯j+x¯)[i=j+1n1χαi(x¯i)]\displaystyle=\left[\prod_{i=1}^{j-1}\chi_{\alpha_{i}}(\bar{x}_{i})\right]\chi_{\alpha_{j}}(\bar{x}_{j}+\bar{x})\left[\prod_{i=j+1}^{n-1}\chi_{\alpha_{i}}(\bar{x}_{i})\right]
=[i=1nχαi(x¯i)]χαj(x¯)\displaystyle=\left[\prod_{i=1}^{n}\chi_{\alpha_{i}}(\bar{x}_{i})\right]\chi_{\alpha_{j}}(\bar{x})

for all x1,,xn,x𝔬x_{1},\dots,x_{n},x\in\mathfrak{o} as desired.

This finishes our proof that there is a unique shallow character of P+P_{+} satisfying (2.4). To see that every shallow character of P+P_{+} is of this form, we note Lemma 3 says that its restrictions to shallow affine root groups must satisfy (2.3). ∎

Corollary 5.

Suppose that for each shallow affine root α\alpha, we are given an additive character

χα:𝔣×.\chi_{\alpha}:\mathfrak{f}\to\mathbb{C}^{\times}.

Suppose further that χα\chi_{\alpha} is trivial whenever α\alpha is decomposable as a shallow affine root. Then there exists a unique shallow character χ:P+/P1×\chi:P_{+}/P_{1}\to\mathbb{C}^{\times} such that

χ(uα(x)P1)=χα(x¯)\chi(u_{\alpha}(x)P_{1})=\chi_{\alpha}(\bar{x})

for all x𝔬x\in\mathfrak{o} and shallow affine roots α\alpha.

Proof.

By the previous theorem, we only need to show that given any shallow affine roots α,β\alpha,\beta we have the following relations:

1=i,jχiα+jβ(Cαβijx¯iy¯j),1=\prod_{i,j}\chi_{i\alpha+j\beta}(C_{\alpha\beta ij}\bar{x}^{i}\bar{y}^{j}), (2.8)

where the product is in increasing order over all i,j>0i,j>0 such that iα+jβi\alpha+j\beta is a shallow affine root. But this is true because each iα+jβi\alpha+j\beta is a decomposable shallow affine root, and thus each χiα+jβ\chi_{i\alpha+j\beta} is trivial. Thus (2.8) naturally holds. ∎

2.3 The space of shallow characters

Let 𝖵ˇ\check{\mathsf{V}} be the set of all shallow characters of P+P_{+}. Then 𝖵ˇ\check{\mathsf{V}} has a natural abelian group structure given by

(χ1+χ2)(g)=χ1(g)χ2(g).(\chi_{1}+\chi_{2})(g)=\chi_{1}(g)\cdot\chi_{2}(g).

Moreover, the group 𝖵ˇ\check{\mathsf{V}} can be endowed with the structure of a 𝔣\mathfrak{f}-vector space as shown below: The finite group P+/P1P_{+}/P_{1} is generated by subgroups of the form

UαP1/P1Uα/Uα+1𝔣U_{\alpha}P_{1}/P_{1}\cong U_{\alpha}/U_{\alpha+1}\cong\mathfrak{f}

for shallow affine roots α\alpha. Once a pinning of GG has been chosen, there is a natural action of 𝔣\mathfrak{f} on each of these subgroups by setting

z¯uα(x)P1:=uα(zx)P1\bar{z}\cdot u_{\alpha}(x)P_{1}:=u_{\alpha}(zx)P_{1}

for all x,z𝔬x,z\in\mathfrak{o} and shallow affine roots α\alpha. This action can be extended to the full group P+/P1P_{+}/P_{1} via distribution by setting

z¯(uα(x)uβ(y)P1)=uα(zx)uβ(zy)P1\bar{z}\cdot(u_{\alpha}(x)u_{\beta}(y)P_{1})=u_{\alpha}(zx)u_{\beta}(zy)P_{1}

for all x,y,z𝔬x,y,z\in\mathfrak{o} and shallow affine roots α,β\alpha,\beta. This in turn endows the abelianization

𝖵:=P+/P1[P+/P1,P+/P1]\mathsf{V}:=\frac{P_{+}/P_{1}}{[P_{+}/P_{1},P_{+}/P_{1}]}

with the structure of a 𝔣\mathfrak{f}-vector space spanned by vectors 𝗏α\mathsf{v}_{\alpha}, the image of uα(1)P1u_{\alpha}(1)P_{1} under the quotient P+/P1𝖵P_{+}/P_{1}\to\mathsf{V}. Finally, this action endows 𝖵ˇ\check{\mathsf{V}} with the structure of a 𝔣\mathfrak{f}-vector space with 𝔣\mathfrak{f}-action given via

[z¯χ](gP1):=χ(z¯1gP1).[\bar{z}\cdot\chi](gP_{1}):=\chi(\bar{z}^{-1}\cdot gP_{1}).

Thus, we have shown that 𝖵ˇ\check{\mathsf{V}} is a 𝔣\mathfrak{f}-vector space.

2.3.1 Epipelagic characters

Recall that for real number 0<r<10<r<1, we say that a shallow affine root α\alpha has depth rr provided that α(λ)=r\alpha(\lambda)=r. We now say that a shallow character χ𝖵ˇ\chi\in\check{\mathsf{V}} has depth rr provided that the following hold:

  • χα\chi_{\alpha} is non-trivial for some shallow affine root α\alpha of depth rr.

  • χα\chi_{\alpha} is trivial for all shallow affine roots α\alpha of depth greater than rr.

The minimal depth α(λ)=r\alpha(\lambda)=r for shallow affine roots α\alpha is r=r1r=r_{1}, the index of the pro-unipotent radical P+=Pr1P_{+}=P_{r_{1}} in the Moy-Prasad filtration. The affine roots at this depth are said to be epipelagic, and since any epipelagic affine root is necessarily indecomposable as a shallow affine root, Corollary 5 implies that the set of all shallow characters of depth r1r_{1} form a non-trivial subspace of 𝖵ˇ\check{\mathsf{V}}, denoted

𝖵ˇ+:=𝖵ˇr1,\check{\mathsf{V}}_{+}:=\check{\mathsf{V}}_{r_{1}},

whose dimension is equal to the non-zero number of epipelagic affine roots. More generally, for all real numbers 0<r<10<r<1, we let

𝖵ˇr:={χ𝖵χ is trivial on Ps for all s>r}\check{\mathsf{V}}_{r}:=\{\chi\in\mathsf{V}\mid\text{$\chi$ is trivial on $P_{s}$ for all $s>r$}\}

be the subspace of all shallow characters of depth at most rr.

3 Supercuspidal Representations

Recall that a smooth representation of GG is a group homomorphism

π:GGL(V),\pi:G\to\operatorname{GL}(V),

where VV is a complex vector space, such that for every vVv\in V there is a compact open subgroup HGH\subseteq G such that π(g)v=v\pi(g)v=v for every gHg\in H. We say that a smooth representation π\pi is supercuspidal is every matrix coefficient of GG is compactly supported modulo the center Z(G)Z(G). We will now investigate which shallow characters of P+P_{+} give rise to supercuspidal representations of GG via compact induction.

3.1 Compact Induction

In this section we will recall some basic facts about compact induction: Let χ:P+/P1×\chi:P_{+}/P_{1}\to\mathbb{C}^{\times} be a shallow character of P+P_{+}, and consider the compactly-induced representation of GG

π(χ):=indP+G(χ)={ϕ:G|ϕ(hg)=χ(h)ϕ(g)ϕ compactly supported},\pi(\chi):=\operatorname{ind}_{P_{+}}^{G}(\chi)={\small\left\{\phi:G\to\mathbb{C}~{}\left|~{}\begin{gathered}\text{$\phi(hg)=\chi(h)\cdot\phi(g)$}\\ \text{$\phi$ compactly supported}\end{gathered}\right\}\right.},

with GG-action given by right translations:

[nϕ](g):=ϕ(gn)[n\cdot\phi](g):=\phi(gn)

for all n,gGn,g\in G. Given any nGn\in G, we set P+n:=nP+n1{}^{n}P_{+}:=nP_{+}n^{-1} and let χn{}^{n}\chi be the conjugate character of P+n{}^{n}P_{+} given by setting

χn(g):=χ(n1gn){}^{n}\chi(g):=\chi(n^{-1}gn)

for all gP+ng\in{}^{n}P_{+}. We then define the intertwining set to be

(G,P+,χ):={nGχnχ on P+nP+}.\mathscr{I}(G,P_{+},\chi):=\{n\in G\mid\text{${}^{n}\chi\cong\chi$ on ${}^{n}P_{+}\cap P_{+}$}\}.

Then we have the following basic result:

Lemma 6.

Let χ:P+/P1×\chi:P_{+}/P_{1}\to\mathbb{C}^{\times} be a shallow character of P+P_{+}. Then the following are equivalent:

  1. a.

    (G,P+,χ)=Pχ\mathscr{I}(G,P_{+},\chi)=P_{\chi}.

  2. b.

    π(χ)\pi(\chi) is irreducible.

  3. c.

    π(χ)\pi(\chi) is supercuspidal.

Recall that the parahoric subgroup PP normalizes Moy-Prasad subgroups P+,P1P_{+},P_{1}, and so the conjugate character χn{}^{n}\chi is then a shallow charater of P+P_{+} for any nPn\in P. We therefore consider the stabilizer of χ\chi in PP:

Pχ:={nNχn=χ}(G,P+,χ).P_{\chi}:=\{n\in N\mid{}^{n}\chi=\chi\}\subseteq\mathscr{I}(G,P_{+},\chi).

The finite quotient Pχ/P+P_{\chi}/P_{+} has order equal to the dimension of the semisimple intertwining algebra

𝒜χ:=EndPχ(indP+Pχ(χ)).\mathscr{A}_{\chi}:=\operatorname{End}_{P_{\chi}}(\operatorname{ind}_{P_{+}}^{P_{\chi}}(\chi)).

There is a bijection ρχρ\rho\mapsto\chi_{\rho} between equivalence classes of irreducible 𝒜χ\mathscr{A}_{\chi}-modules and the irreducible PχP_{\chi} representations appearing in the isotypic decomposition

indP+Pχ(χ)=ρdim(ρ)χρ.\operatorname{ind}_{P_{+}}^{P_{\chi}}(\chi)=\bigoplus_{\rho}\dim(\rho)\cdot\chi_{\rho}.

Then we have the following result, whose proof can be found in [4, §2.1]:

Lemma 7.

Let χ:P+/P1×\chi:P_{+}/P_{1}\to\mathbb{C}^{\times} be a shallow character of P+P_{+}. If (G,P+,χ)=Pχ\mathscr{I}(G,P_{+},\chi)=P_{\chi}, then we have the following isotypic decomposition:

π(χ)=ρdim(ρ)indPχG(χρ),\pi(\chi)=\bigoplus_{\rho}\dim(\rho)\cdot\operatorname{ind}_{P_{\chi}}^{G}(\chi_{\rho}),

where the direct sum is over all simple 𝒜χ\mathscr{A}_{\chi} modules ρ\rho. Moreover, each compactly induced representation

π(χ,ρ):=indPχG(χρ)\pi(\chi,\rho):=\operatorname{ind}_{P_{\chi}}^{G}(\chi_{\rho})

are inequivalent irreducible supercuspidal representations of GG.

3.2 Supercuspidal representations coming from shallow characters

Let μ\mu be any point in the apartment 𝒜\mathcal{A}. For all positive real numbers s>0s>0, let

𝖵μ,s:=span𝔣{𝗏α𝖵0<α(λ)<1 and α(μ)s}\mathsf{V}_{\mu,s}:=\operatorname{span}_{\mathfrak{f}}\{\mathsf{v}_{\alpha}\in\mathsf{V}\mid\text{$0<\alpha(\lambda)<1$ and $\alpha(\mu)\geq s$}\}

be the 𝔣\mathfrak{f}-span of the vectors 𝗏α\mathsf{v}_{\alpha} for shallow affine roots α\alpha such that α(μ)s\alpha(\mu)\geq s. Then we have the following sufficient condition for constructing supercuspidal representations:

Proposition 8.

Let χ𝖵ˇr\chi\in\check{\mathsf{V}}_{r} be any depth rr shallow character such that the following holds:

  • ()(*)

    If nNG(T)n\in N_{G}(T) and χ\chi identically vanishes on 𝖵nλ,s\mathsf{V}_{n\lambda,s} for all s>rs>r, then nλ=λn\lambda=\lambda.

Then (G,P+,χ)=Pχ\mathscr{I}(G,P_{+},\chi)=P_{\chi}.

Proof.

Let χ𝖵ˇr\chi\in\check{\mathsf{V}}_{r} be a depth rr shallow character of P+P_{+} satisfying ()(*). Since PP contains an Iwahori subgroup, the affine Bruhat decomposition [3] implies that in order to show that (G,P+,χ)=Pχ\mathscr{I}(G,P_{+},\chi)=P_{\chi}, it will be sufficient to consider nNG(T)n\in N_{G}(T) and show that if

χn=χ on P+nP+.{}^{n}\chi=\chi\text{ on }{}^{n}P_{+}\cap P_{+}. (3.1)

then nPn\in P.

Let nNG(T)n\in N_{G}(T) be such that (3.1) holds, and fix a real number s>rs>r. It is certainly true that

χn=χ on PsnP+{}^{n}\chi=\chi\text{ on }{}^{n}P_{s}\cap P_{+} (3.2)

for the Moy-Prasad subgroup PsPP_{s}\subseteq P. Let α\alpha be any shallow root such that α(nλ)s\alpha(n\lambda)\geq s. Since it has depth rr, χ\chi must then be trivial on Un1αPsU_{n^{-1}\alpha}\subseteq P_{s}. Therefore, χα\chi_{\alpha} must be the trivial additive character, since (3.2) requires that

χα(x¯)=χ(uα(x))=χn(uα(x))=χ(un1α(±x))=1\chi_{\alpha}(\bar{x})=\chi(u_{\alpha}(x))={}^{n}\chi(u_{\alpha}(x))=\chi(u_{n^{-1}\alpha}(\pm x))=1

for all x𝔬x\in\mathfrak{o}. But this holds for all s>rs>r and all shallow affine roots α\alpha such that α(nλ)s\alpha(n\lambda)\geq s, and thus χ\chi vanishes identically on 𝖵nλ,s\mathsf{V}_{n\lambda,s} for all s>rs>r. Consequently, ()(*) implies that nλ=λn\lambda=\lambda so that nPn\in P. ∎

Remark.

In the remainder of this subsection we study condition ()(*) of Proposition 8 in further detail. In particular, we first show in §3.2.1 how ()(*) is a necessary condition for constructing simple supercuspidal representations of GG. Then in §3.2.2 we show how, when leaving the epipelagic case, condition ()(*) is no longer necessary for constructing supercuspidal representations of GG.

3.2.1 Simple supercuspidal representations

In this subsubsection only, we will make the additional assumption that λ\lambda is the barycenter of the fundamental open alcove in 𝒜\mathcal{A} bonded by Δ\Delta. If

1=m0α0+m1α1++mα1=m_{0}\alpha_{0}+m_{1}\alpha_{1}+\cdots+m_{\ell}\alpha_{\ell} (3.3)

is the minimal integral relation on simple affine roots with mi>0m_{i}>0, then λ\lambda is the unique point such that for all simple αiΔ\alpha_{i}\in\Delta,

αi(λ)=1/h,\alpha_{i}(\lambda)=1/h,

where h:=m0+m1++mh:=m_{0}+m_{1}+\cdots+m_{\ell} is the Coxeter number of RR. In this case, the parahoric subgroup P=GλP=G_{\lambda} is an Iwahori subgroup of GG.

Lemma 9.

Let λ\lambda be the barycenter of the fundamental open alcove in 𝒜\mathcal{A}. Then for any nNG(T)n\in N_{G}(T) such that nλλn\lambda\neq\lambda, there must exist a simple affine root αiΔ\alpha_{i}\in\Delta such that αi(nλ)>1/h\alpha_{i}(n\lambda)>1/h.

Proof.

Let nNG(T)n\in N_{G}(T) be such that nλλn\lambda\neq\lambda. The difference μ=λnλ\mu=\lambda-n\lambda belongs to the translation group

E:=Hom(k,T),E:=\mathbb{R}\otimes_{\mathbb{Z}}\operatorname{Hom}(k,T),

so that we can write μ=sc\mu=sc for some real number s>0s>0 and non-trivial cocharacter cHom(k,T)c\in\operatorname{Hom}(k,T). For all simple affine roots αiΔ\alpha_{i}\in\Delta, we have

αi(nλ)=αi(λ+sc)=αi(λ)+sai,c,\alpha_{i}(n\lambda)=\alpha_{i}(\lambda+sc)=\alpha_{i}(\lambda)+s\langle a_{i},c\rangle,

where aia_{i} is the gradient of αi\alpha_{i}. Since Δ\Delta forms a base of the affine root system, the gradients a0,a1,,aa_{0},a_{1},\dots,a_{\ell} form a spanning set of the \ell-dimensional vector space

E:=Hom(T,k),E^{*}:=\mathbb{R}\otimes_{\mathbb{Z}}\operatorname{Hom}(T,k),

which is dual to EE under the natural pairing ,\langle\cdot,\cdot\rangle. Therefore, there must be some αi\alpha_{i} such that ai,c0\langle a_{i},c\rangle\neq 0. Without loss of generality, we can assume that ai,c>0\langle a_{i},c\rangle>0 so that αi(nλ)>1/h\alpha_{i}(n\lambda)>1/h; otherwise, if aj,c0\langle a_{j},c\rangle\leq 0 for all αjΔ\alpha_{j}\in\Delta, then (3.3) implies that

0=m0a0,c+m1a1,c++ma,c<0,0=m_{0}\langle a_{0},c\rangle+m_{1}\langle a_{1},c\rangle+\cdots+m_{\ell}\langle a_{\ell},c\rangle<0,

a contradiction. ∎

Lemma 10.

Let λ\lambda be the barycenter of the fundamental open alcove in 𝒜\mathcal{A}. Then given any non-empty, proper subset

I{0,1,,},I\subsetneq\{0,1,\dots,\ell\},

there must exist an element nNG(T)n\in N_{G}(T) such that αi(nλ)<0\alpha_{i}(n\lambda)<0 for all iIi\in I.

Proof.

Consider the affine Weyl group

W:=NG(T)/T0W:=N_{G}(T)/T_{0}

and the subgroup WIW_{I} of WW generated by simple reflections along the simple affine roots αi\alpha_{i} for iIi\in I. Note that WIW_{I} is a non-empty, finite Coxeter group, since II is a non-empty, proper subset of {0,1,,}\{0,1,\dots,\ell\}. Let w:=wIw:=w_{I} be the long element in WIW_{I}; that is, ww is the unique element on WIW_{I} such that wαiw\alpha_{i} is a negative affine root for all iIi\in I. Such an element has order 22, so that

w1α=wαw^{-1}\alpha=w\alpha

for all affine roots α\alpha. Moreover, since an affine root is negative if and only if it takes negative values on the open fundamental alcove, we have

αi(wλ)=(w1αi)(λ)=(wαi)(λ)<0\alpha_{i}(w\lambda)=(w^{-1}\alpha_{i})(\lambda)=(w\alpha_{i})(\lambda)<0

for all iIi\in I. Thus, letting nNG(T)n\in N_{G}(T) be any lift of ww, we are done. ∎

Proposition 11.

Let λ\lambda be the barycenter of the fundamental open alcove in 𝒜\mathcal{A}. Then given any epipelagic character χ𝖵ˇ1/h\chi\in\check{\mathsf{V}}_{1/h}, the following are equivalent:

  1. a.

    χαi\chi_{\alpha_{i}} is non-trivial for all αiΔ\alpha_{i}\in\Delta.

  2. b.

    If nNG(T)n\in N_{G}(T) and χ\chi vanishes identically on 𝖵nλ,s\mathsf{V}_{n\lambda,s} for all s>1/hs>1/h, then nλ=λn\lambda=\lambda.

Proof.

(ab)(a\Rightarrow b): Suppose that χαi\chi_{\alpha_{i}} is non-trivial for all αiΔ\alpha_{i}\in\Delta, and let nNG(T)n\in N_{G}(T). By Lemma 9 there exists some αi\alpha_{i} such that αi(nλ)>1/h\alpha_{i}(n\lambda)>1/h. Since χαi\chi_{\alpha_{i}} is non-trivial, there must exist some s>1/hs>1/h such that χ\chi does not vanish identically on 𝔣𝗏αi𝖵nλ,s\mathfrak{f}\mathsf{v}_{\alpha_{i}}\subseteq\mathsf{V}_{n\lambda,s}.

(¬a¬b)(\neg a\Rightarrow\neg b): Suppose that there exists some simple affine root αiΔ\alpha_{i}\in\Delta such that χαi\chi_{\alpha_{i}} is trivial. Setting

I:={iχαi is non-trivial}{0,1,,}I:=\{i\mid\text{$\chi_{\alpha_{i}}$ is non-trivial}\}\subsetneq\{0,1,\dots,\ell\}

and applying Lemma 10, we see that there must exist some nNG(T)n\in N_{G}(T) such that αi(nλ)<0\alpha_{i}(n\lambda)<0 whenever χαi\chi_{\alpha_{i}} is non-trivial. In this case, for all s>1/hs>1/h, the vector space 𝖵nλ,s\mathsf{V}_{n\lambda,s} is contained within the span of subspaces 𝔣𝗏α\mathfrak{f}\mathsf{v}_{\alpha} for shallow affine roots α\alpha such that χα\chi_{\alpha} is trivial. Thus, χ\chi identically vanishes on 𝖵nλ,s\mathsf{V}_{n\lambda,s} while nλλn\lambda\neq\lambda. ∎

Corollary 12.

Let λ\lambda be the barycenter of the fundamental open alcove in 𝒜\mathcal{A}, and let χ𝖵ˇ1/h\chi\in\check{\mathsf{V}}_{1/h} be any epipelagic character such that χαi\chi_{\alpha_{i}} is non-trivial for all αiΔ\alpha_{i}\in\Delta. Then (G,P+,χ)=Pχ\mathscr{I}(G,P_{+},\chi)=P_{\chi}.

Remark.

In the case given by the above corollary, the supercuspidal representations π(χ,ρ)\pi(\chi,\rho) obtained from compact induction are called simple supercuspidal representations, and they were first studied by Gross-Reeder in [2]. This is a special class of epipelagic representations which were later studied by Reeder-Yu in [4].

3.2.2 A supercuspidal representation of 𝐒𝐩4(2)\operatorname{\bf Sp}_{4}(\mathbb{Q}_{2})

Let G=𝐒𝐩4(k)G=\operatorname{\bf Sp}_{4}(k) be the simply connected Chevalley group consisting of matrices in 𝐒𝐋2(k)\operatorname{\bf SL}_{2}(k) which are fixed under the endomorphism

XQ1(X)1Q,X\mapsto Q^{-1}(X^{{\dagger}})^{-1}Q,

where [xij]=[xji][x_{ij}]^{\dagger}=[x_{ji}] denotes transposition and QQ is the skew-symmetric matrix

Q=[1111].Q=\begin{bmatrix}&&&1\\ &&1\\ &-1\\ -1\end{bmatrix}.

Alternatively, GG is seen as the group of isometries with respect to the Hermitian form given by QQ. We fix the diagonal maximal torus

T={t=[t1t2t3t4]|t1,t2,t3,t42× witht1t4=1 and t2t3=1}T=\left.\left\{t=\begin{bmatrix}t_{1}\\ &t_{2}\\ &&t_{3}\\ &&&t_{4}\end{bmatrix}~{}\right|~{}\begin{gathered}\text{$t_{1},t_{2},t_{3},t_{4}\in\mathbb{Q}_{2}^{\times}$ with}\\ \text{$t_{1}t_{4}=1$ and $t_{2}t_{3}=1$}\end{gathered}\right\}

The root system R=R(G,T)R=R(G,T) of GG relative to TT has type 𝐂2\mathbf{C}_{2} with base given by short root a1(t)=t1/t2a_{1}(t)=t_{1}/t_{2} and long root a2(t)=t2/t3a_{2}(t)=t_{2}/t_{3}. For convenience, we will denote by a0(t)=t4/t1a_{0}(t)=t_{4}/t_{1} the lowest long root in RR relative to this chosen base. A base Δ\Delta of the affine root system of GG relative to TT can be given by the following three affine functionals:

α0\displaystyle\alpha_{0} =a0+1\displaystyle=a_{0}+1
α1\displaystyle\alpha_{1} =a1+0\displaystyle=a_{1}+0
α2\displaystyle\alpha_{2} =a2+0\displaystyle=a_{2}+0

It should be noted that these simple affine roots satisfy the minimal relation

α0+2α1+α2=1.\alpha_{0}+2\alpha_{1}+\alpha_{2}=1.

By fixing a pinning of GG via the following root group morphisms:

ua1(x)\displaystyle\small u_{a_{1}}(x) =[1x11x1]\displaystyle={\begin{bmatrix}1&x&&\\ &1&&\\ &&1&-x\\ &&&1\end{bmatrix}} ua0+a1+a2(x)\displaystyle u_{a_{0}+a_{1}+a_{2}}(x) =[1x11x1]\displaystyle={\begin{bmatrix}1&&&\\ x&1&&\\ &&1&\\ &&-x&1\end{bmatrix}}
ua2(x)\displaystyle u_{a_{2}}(x) =[11x11]\displaystyle={\begin{bmatrix}1&&&\\ &1&x&\\ &&1&\\ &&&1\end{bmatrix}} u2a1+a0(x)\displaystyle u_{2a_{1}+a_{0}}(x) =[11x11]\displaystyle={\begin{bmatrix}1&&&\\ &1&&\\ &x&1&\\ &&&1\end{bmatrix}}
ua1+a2(x)\displaystyle u_{a_{1}+a_{2}}(x) =[1x1x11]\displaystyle={\begin{bmatrix}1&&x&\\ &1&&x\\ &&1&\\ &&&1\end{bmatrix}} ua0+a1(x)\displaystyle u_{a_{0}+a_{1}}(x) =[11x1x1]\displaystyle={\begin{bmatrix}1&&&\\ &1&&\\ x&&1&\\ &x&&1\end{bmatrix}}
u2a2+a1(x)\displaystyle u_{2a_{2}+a_{1}}(x) =[1x111]\displaystyle={\begin{bmatrix}1&&&x\\ &1&&\\ &&1&\\ &&&1\end{bmatrix}} ua0(x)\displaystyle u_{a_{0}}(x) =[111x1]\displaystyle={\begin{bmatrix}1&&&\\ &1&&\\ &&1&\\ x&&&1\end{bmatrix}}

for xkx\in k, we are able to directly compute the structure constants in the Chevalley commutator formulas:

[uα1(y),uα2(x)]=uα1+α2(+xy)u2α1+α2(xy2)[uα1(y),uα0(x)]=uα0+α1(xy)uα0+2α1(xy2)[uα1(y),uα1+α2(x)]=u2α1+α2(+2xy)[uα1(y),uα0+α1(x)]=uα0+2α1(2xy)[uα2(y),uα0+α1(x)]=uα0+α1+α2(xy)uα0+1(x2y)[uα0(y),uα1+α2(x)]=uα0+α1+α2(xy)uα2+1(x2y)[uα1+α2(y),uα0+2α1(x)]=uα1+1(+xy)u2α1+α2+1(+xy2)[uα0+α1(y),u2α1+α2(x)]=uα1+1(xy)uα0+2α1+1(+xy2)[uα1+α2(y),uα0+α1+α2(x)]=uα2+1(2xy)[uα0+α1(y),uα0+α1+α2(x)]=uα0+1(+2xy)[u2α1+α2(y),uα0+α1+α2(x)]=uα1+α2+1(xy)uα2+2(+x2y)[uα0+2α1(y),uα0+α1+α2(x)]=uα0+α1+1(+xy)uα0+2(+x2y)}\left.\begin{aligned} \small{}[u_{\alpha_{1}}(y),u_{\alpha_{2}}(x)]&=u_{\alpha_{1}+\alpha_{2}}(+xy)u_{2\alpha_{1}+\alpha_{2}}(-xy^{2})\\ [u_{\alpha_{1}}(y),u_{\alpha_{0}}(x)]&=u_{\alpha_{0}+\alpha_{1}}(-xy)u_{\alpha_{0}+2\alpha_{1}}(-xy^{2})\\[8.0pt] [u_{\alpha_{1}}(y),u_{\alpha_{1}+\alpha_{2}}(x)]&=u_{2\alpha_{1}+\alpha_{2}}(+2xy)\\ [u_{\alpha_{1}}(y),u_{\alpha_{0}+\alpha_{1}}(x)]&=u_{\alpha_{0}+2\alpha_{1}}(-2xy)\\[8.0pt] [u_{\alpha_{2}}(y),u_{\alpha_{0}+\alpha_{1}}(x)]&=u_{\alpha_{0}+\alpha_{1}+\alpha_{2}}(-xy)u_{\alpha_{0}+1}(-x^{2}y)\\ [u_{\alpha_{0}}(y),u_{\alpha_{1}+\alpha_{2}}(x)]&=u_{\alpha_{0}+\alpha_{1}+\alpha_{2}}(-xy)u_{\alpha_{2}+1}(-x^{2}y)\\[8.0pt] [u_{\alpha_{1}+\alpha_{2}}(y),u_{\alpha_{0}+2\alpha_{1}}(x)]&=u_{\alpha_{1}+1}(+xy)u_{2\alpha_{1}+\alpha_{2}+1}(+xy^{2})\\ [u_{\alpha_{0}+\alpha_{1}}(y),u_{2\alpha_{1}+\alpha_{2}}(x)]&=u_{\alpha_{1}+1}(-xy)u_{\alpha_{0}+2\alpha_{1}+1}(+xy^{2})\\[8.0pt] [u_{\alpha_{1}+\alpha_{2}}(y),u_{\alpha_{0}+\alpha_{1}+\alpha_{2}}(x)]&=u_{\alpha_{2}+1}(-2xy)\\ [u_{\alpha_{0}+\alpha_{1}}(y),u_{\alpha_{0}+\alpha_{1}+\alpha_{2}}(x)]&=u_{\alpha_{0}+1}(+2xy)\\[8.0pt] [u_{2\alpha_{1}+\alpha_{2}}(y),u_{\alpha_{0}+\alpha_{1}+\alpha_{2}}(x)]&=u_{\alpha_{1}+\alpha_{2}+1}(-xy)u_{\alpha_{2}+2}(+x^{2}y)\\ [u_{\alpha_{0}+2\alpha_{1}}(y),u_{\alpha_{0}+\alpha_{1}+\alpha_{2}}(x)]&=u_{\alpha_{0}+\alpha_{1}+1}(+xy)u_{\alpha_{0}+2}(+x^{2}y)\end{aligned}\right\} (3.4)

for any x,y𝔬x,y\in\mathfrak{o}.

Suppose that λ\lambda is contained within the closure of the alcove bounded by the vanishing hyperplanes of the simple affine roots in Δ\Delta. The set of positive affine roots which take value at most 11 at λ\lambda is therefore

{α0,α1,α2,α0+α1,α1+α2,α0+2α1,α0+α1+α2,2α1+α2},\{\alpha_{0},\alpha_{1},\alpha_{2},\alpha_{0}+\alpha_{1},\alpha_{1}+\alpha_{2},\alpha_{0}+2\alpha_{1},\alpha_{0}+\alpha_{1}+\alpha_{2},2\alpha_{1}+\alpha_{2}\},

and those which take non-zero value at λ\lambda form the shallow affine roots. Thus, in order to define a shallow character

χ:P+/P1×,\chi:P_{+}/P_{1}\to\mathbb{C}^{\times},

one only needs to verify that the restrictions to the shallow affine root groups satisfy the following relations coming from the commutators in (3.4):

{1=χα1+α2(xy)χ2α1+α2(xy2)if α1,α2 are shallow1=χα0+α1(xy)χα0+2α1(xy2)if α0,α1 are shallow1=χα0+α1+α2(xy)if α2,α0+α1 are shallow1=χα0+α1+α2(xy)if α0,α1+α2 are shallow\begin{cases}1=\chi_{\alpha_{1}+\alpha_{2}}(xy)\cdot\chi_{2\alpha_{1}+\alpha_{2}}(xy^{2})&\text{if $\alpha_{1},\alpha_{2}$ are shallow}\\ 1=\chi_{\alpha_{0}+\alpha_{1}}(xy)\cdot\chi_{\alpha_{0}+2\alpha_{1}}(xy^{2})&\text{if $\alpha_{0},\alpha_{1}$ are shallow}\\ 1=\chi_{\alpha_{0}+\alpha_{1}+\alpha_{2}}(xy)&\text{if $\alpha_{2},\alpha_{0}+\alpha_{1}$ are shallow}\\ 1=\chi_{\alpha_{0}+\alpha_{1}+\alpha_{2}}(xy)&\text{if $\alpha_{0},\alpha_{1}+\alpha_{2}$ are shallow}\end{cases} (3.5)

for all x,y𝔣x,y\in\mathfrak{f}.

Example 13.

Suppose that the residue field of kk has order q=2q=2, and let λ\lambda be the barycenter of the open alcove. Then consider the shallow character

χ:P+/P1×\chi:P_{+}/P_{1}\to\mathbb{C}^{\times}

given by additive characters

αχα(1)α01α1+1α2+1α0+α11α1+α21α0+2α11α0+α1+α2+12α1+α21\begin{array}[]{|c|c|}\hline\cr\alpha&\chi_{\alpha}(1)\\ \hline\cr\hline\cr\alpha_{0}&-1\\ \alpha_{1}&+1\\ \alpha_{2}&+1\\ \hline\cr\alpha_{0}+\alpha_{1}&-1\\ \alpha_{1}+\alpha_{2}&-1\\ \hline\cr\alpha_{0}+2\alpha_{1}&-1\\ \alpha_{0}+\alpha_{1}+\alpha_{2}&+1\\ 2\alpha_{1}+\alpha_{2}&-1\\ \hline\cr\end{array}

Note that χ\chi has depth 3/43/4, but if

n1=[1111]NG(T)n_{1}=\begin{bmatrix}&1\\ -1\\ &&&-1\\ &&1\end{bmatrix}\in N_{G}(T)

is a lift of the simple reflection about the vanishing hyperplane of α1\alpha_{1}, then for any s>3/4s>3/4

𝖵n1λ,s𝔣𝗏α0+α1+α2,\mathsf{V}_{n_{1}\lambda,s}\subseteq\mathfrak{f}\mathsf{v}_{\alpha_{0}+\alpha_{1}+\alpha_{2}},

over which χ\chi vanishes identically; thus χ\chi does not statisfy condition ()(*) in Proposition 8. Despite this, we see that χ\chi compactly induces to give a supercuspidal representation of 𝐒𝐩4(k)\operatorname{\bf Sp}_{4}(k). To see this, we first make the following observations:

  • If α\alpha is a short affine root, then nαn\alpha is also short for all nNG(T)n\in N_{G}(T).

  • The only positive, short affine roots α\alpha for which χα(1)=1\chi_{\alpha}(1)=-1 are α0+α1\alpha_{0}+\alpha_{1} and α1+α2\alpha_{1}+\alpha_{2}.

  • For any nNG(T)n\in N_{G}(T), either n(α0+α1)n(\alpha_{0}+\alpha_{1}) or n(α1+α2)n(\alpha_{1}+\alpha_{2}) is a positive affine root.

Consequently, for any nNG(T)n\in N_{G}(T),

χn=χ on P+nP{}^{n}\chi=\chi\text{ on }{}^{n}P_{+}\cap P

only if nn either fixes both α0+α1\alpha_{0}+\alpha_{1} and α1+α2\alpha_{1}+\alpha_{2} or swaps them. If nn fixes both short affine roots, then either

{n(α0)=α02mn(2α1+α2)=2α1+α2+2m}or{n(α0)=2α0+α12mn(2α1+α2)=α2+2m}\left\{\begin{array}[]{lcl}n(\alpha_{0})&=&\alpha_{0}-2m\\ n(2\alpha_{1}+\alpha_{2})&=&2\alpha_{1}+\alpha_{2}+2m\end{array}\right\}\quad\text{or}\quad\left\{\begin{array}[]{lcl}n(\alpha_{0})&=&2\alpha_{0}+\alpha_{1}-2m\\ n(2\alpha_{1}+\alpha_{2})&=&\alpha_{2}+2m\end{array}\right\}

holds for some mm\in\mathbb{Z}; if nn swaps the short affine roots, then either

{n(α0)=2α1+α22m+1n(α0+2α1)=α2+2m+1}or{n(α0)=α22m+1n(α0+2α1)=2α1+α2+2m+1}\left\{\begin{array}[]{lcl}n(\alpha_{0})&=&2\alpha_{1}+\alpha_{2}-2m+1\\ n(\alpha_{0}+2\alpha_{1})&=&\alpha_{2}+2m+1\end{array}\right\}\quad\text{or}\quad\left\{\begin{array}[]{lcl}n(\alpha_{0})&=&\alpha_{2}-2m+1\\ n(\alpha_{0}+2\alpha_{1})&=&2\alpha_{1}+\alpha_{2}+2m+1\end{array}\right\}

holds for some mm\in\mathbb{Z}. In all cases, if nn does not act trivially on the affine roots, there exists some long shallow affine root α\alpha such that nαn\alpha is also a positive affine root with

1=χα(1)χnα(1)=1.-1=\chi_{\alpha}(1)\neq\chi_{n\alpha}(1)=1.

Thus, given any nNG(T)n\in N_{G}(T), there exists some positive affine root α\alpha such that χα(1)χnα(1)\chi_{\alpha}(1)\neq\chi_{n\alpha}(1). Finally, the affine Bruhat decomposition

G=PNG(T)PG=PN_{G}(T)P

implies that (G,P+,χ)=Pχ=P+\mathscr{I}(G,P_{+},\chi)=P_{\chi}=P_{+}, where the last equality holds since q=2q=2. Hence, we have constructed a supercuspidal representation π(χ)\pi(\chi) of Sp4(k)\operatorname{Sp}_{4}(k) coming from a shallow character of II not satisfying condition ()(*) in Proposition 8.

References

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